Optical resonator
1. What a Resonator (Cavity) Is
Optical resonator / cavity = two parallel mirrors ( highly reflective %, partially transmitting %) enclosing the gain medium, providing feedback and mode selection.
Without resonator, stimulated photons leave — no amplification; with resonator, photons bounce many times ⇒ photon density builds up ⇒ gain > loss ⇒ laser oscillation.
2. Conditions for Lasing (gain + resonator)
- Threshold condition:
where is gain coefficient (∝ ), internal loss, cavity length, mirror reflectivities.
- Phase condition: round-trip phase ⇒
⇒ only longitudinal modes spaced
(for linear Fabry-Perot) oscillate within gain linewidth.
Resonator selects one axial direction ⇒ directionality.
3. Types of Cavities
- Fabry-Perot (plane-parallel): simple, but unstable if misaligned.
- Confocal / concentric / hemispherical: curved mirrors for stability (stability condition where ).
- Ring cavity: three mirrors in triangle (used in gyros).
Active medium often at mode waist.
4. Functions of Resonator (exam list)
- Feedback — returns photons to gain medium for further stimulated emission (amplification loop).
- Mode selection — only satisfying and within gain bandwidth oscillate ⇒ spectral narrowing (monochromatic).
- Direction selection — photons off-axis walk out after few bounces ⇒ only axial photons stay ⇒ collimated beam.
- Coherence building — many round trips phase-lock photons ⇒ high coherence.
5. Worked Note
He-Ne cavity L=30 cm: Δν=c/2L=500 MHz; gain linewidth ~1.5 GHz ⇒ ~3 modes can oscillate; etalon selects one.
Ruby cavity L=10 cm: mode spacing c/2L=1.5 GHz; gain linewidth ~300 GHz ⇒ many modes, but Q-switch selects.
Threshold: if R1=100%, R2=95%, L=30 cm, α≈0.01 cm⁻¹: need g> α + ln(1/0.95)/0.6 ≈0.01+0.085≈0.095 cm⁻¹.
6. Exam Points
- Define resonator and draw Fabry-Perot cavity — 5 marks, very frequent.
- Explain feedback and threshold — 5 marks, very frequent.
- Phase condition , mode spacing — 5 marks, frequent.
- Functions (feedback, mode/direction selection) — 5 marks, very frequent.